Cryptography Reference
In-Depth Information
11.4 Information Theory of Cryptosystems
Where is the wisdom we have lost in knowledge?
Where is the knowledge we have lost in information?
T.S. Eliot (1888-1965), Anglo-American poet, critic, and dramatist
— from The Rock (1934)
When we defined conditional entropyin Equation (11.3) on page 431, we
looked at a cryptological context. It is this interpretation upon which we now
concentrate. In fact, the quantitydefined in that context for Equation (11.3) is
called key equivocation .
Key Equivocation
The entropy of cryptosystems is a key feature upon which we will focus
herein. A cryptosystem may be defined by parameters that include the keyspace
K
(as well as encryption and
decryption transformations), and certain probability distributions given as fol-
lows. Each plaintext unit, m
, the message space
M
, the ciphertext space
C
M
, has a certain probabilityof occurring, and
the choice of key k
K
is assumed to be independent of the choice of m , with
probabilityof a given k
K
also having a probabilitydistribution from which
it follows that
H (
K
,
M
)= H (
K
)+ H (
M
)
(see part 1 of The Role of Independence on page 432). Also, the possible c
C
have a probabilitydistribution that depends on the probabilitydistributions for
M
K
and
. Given this setup, the keyequivocation satisfies
K | C
K
M
C
H (
)= H (
)+ H (
)
H (
) ,
(11.8)
which is a measure of how much information about the keyis revealed bythe
ciphertext.
Example 11.7 Let
M
=
{
s 1 ,s 2 ,s 3 ,s 4 }
with probabilities,
p s 1 =0 . 1 , s 2 =0 . 2 , s 3 =0 . 3 , and p s 4 =0 . 4;
K
=
{
k 1 ,k 2 ,k 3 }
with probabilities,
p k 1 =0 . 3 , k 2 =0 . 3 , and p k 3 =0 . 4;
and
.
If E k is the enciphering transformation for a given k
C
=
{
c 1 ,c 2 ,c 3 ,c 4 }
K
, and
E k 1 ( s 1 )= c 1 ; E k 1 ( s 2 )= c 2 ; E k 1 ( s 3 )= c 3 ; E k 1 ( s 4 )= c 4
E k 2 ( s 1 )= c 2 ; E k 2 ( s 2 )= c 3 ; E k 2 ( s 3 )= c 4 ; E k 2 ( s 4 )= c 1
E k 3 ( s 1 )= c 3 ; E k 3 ( s 2 )= c 4 ; E k 3 ( s 3 )= c 1 ; E k 3 ( s 4 )= c 2
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